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3. Differential operators

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1 3. Differential operators
Gradient 1- Definition. f(x,y,z) is a differentiable scalar field 2 – Physical meaning: is the local variation of f along dr. Particularly, grad f is perpendicular to the line f = ctt. Summer School 2007 B. Rossetto

2 3. Differential operators
Divergence 1 – Definition is a differentiable vector field x x+dx 2 – Physical meaning is associated to local conservation laws: for example, we’ll show that if the mass of fluid (or of charge) outcoming from a domain is equal to the mass entering, then is the fluid velocity (or the current) vectorfield Summer School 2007 B. Rossetto

3 3. Differential operators
Curl 1 – Definition. is a differentiable vector field 2 – Physical meaning: is related to the local rotation of the vectorfield: If is the fluid velocity vectorfield Summer School 2007 B. Rossetto

4 3. Differential operators
Laplacian: definitions 1 – Scalar Laplacian. f(x,y,z) is a differentiable scalar field 2 – Vector Laplacian. is a differentiable vector field Summer School 2007 B. Rossetto

5 3. Differential operators
Laplacian: physical meaning f(x) As a second derivative, the one-dimensional Laplacian operator is related to minima and maxima: when the second derivative is positive (negative), the curvature is concave (convexe). convex concave x In most of situations, the 2-dimensional Laplacian operator is also related to local minima and maxima. If vE is positive: E Summer School 2007 B. Rossetto

6 3. Differential operators
Summary Operator grad div curl Laplacian is a vector a scalar (resp. a vector) concerns a scalar field a vector field (resp. a vector field) Definition resp. Summer School 2007 B. Rossetto

7 3. Differential operators
Cylindrical coordinates Summer School 2007 B. Rossetto

8 3. Differential operators
Cylindrical coordinates Summer School 2007 B. Rossetto

9 3. Differential operators
Spherical coordinates Summer School 2007 B. Rossetto

10 3. Differential operators
Conservative vectorfield Theorem. If there exists f such that then H P Consequently, the value of the integral doesn’t depend on the path, but only on its beginning A and its end B. We say that the vectorfield is conservative Proof. Summer School 2007 B. Rossetto

11 3. Differential operators
1st Stokes formula: vectorfield global circulation Theorem. If S(C) is any oriented surface delimited by C: S(C) C Sketch of proof. y Vy . Vx . . P x . … and then extend to any surface delimited by C. Summer School 2007 B. Rossetto

12 3. Differential operators
2nd Stokes formula: global conservation laws Theorem. If V(C) is the volume delimited by S Sketch of proof. Flow through the oriented elementary planes x = ctt and x+dx = ctt : x x+dx -Vx(x,y,z).dydz + Vx (x+dx,y,z).dydz and then extend this expression to the lateral surface of the cube. Other expression: extended to the vol. of the elementary cube: Summer School 2007 B. Rossetto

13 3. Differential operators
Vector identities Use Einstein convention and Levi-Civita symbol to show them curl(grad f) = 0 Summer School 2007 B. Rossetto


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